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CN113094927B - Method for realizing multi-channel information coding by using novel optical film - Google Patents

Method for realizing multi-channel information coding by using novel optical film Download PDF

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CN113094927B
CN113094927B CN202110450216.8A CN202110450216A CN113094927B CN 113094927 B CN113094927 B CN 113094927B CN 202110450216 A CN202110450216 A CN 202110450216A CN 113094927 B CN113094927 B CN 113094927B
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邓娟
鄢波
高凡
唐轶峻
蔡萍根
陈乃波
吕斌
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Abstract

The invention discloses a method for realizing multi-channel information coding by using a novel optical film, which comprises the following steps: 1) Constructing a nanostructure unit; 2) Optimizing the structural parameters of the nanostructure elements according to the wavelength lambda of incident light; 3) Constructing a nanostructure array comprising a plurality of nanostructure elements; set to the polarization direction alpha 1 Linearly polarized light of which the value is not less than pi/2 is incident to the nano structure array and then passes through the alpha direction of the light transmission axis 2 A polarization analyzer of =0 capable of encoding a first image on the nanostructure array; linearly polarized light with the polarization direction unchanged is incident to the nanostructure array and then is transmitted to alpha from the light transmission axis direction 2 A polarization analyzer of = pi/4, capable of encoding a second image on the surface of the nanostructure array; off-normal direction alpha 1 Linearly polarized light of which the frequency is not less than-pi/8 is incident to the nanostructure array and then passes through the direction alpha of a light transmission axis 2 The analyzer with the color value of = pi/8 can encode a third image on the surface of the nanostructure array, and can be applied to the fields of polarization display, encryption, high-end anti-counterfeiting and the like.

Description

一种利用新型光学薄膜实现多通道信息编码的方法A method for multi-channel information encoding using a novel optical film

技术领域technical field

本发明属于微纳光学和偏振光学技术领域,尤其涉及一种利用新型光学薄膜实现多通道信息编码的方法。The invention belongs to the technical fields of micro-nano optics and polarization optics, and in particular relates to a method for realizing multi-channel information coding by using a novel optical film.

背景技术Background technique

超表面材料是一个由亚波长结构阵列组成的、对光波具有超强调控能力的新型纳米材料。它的出现为实现光电器件的小型化、集成化、高性能提供了一种新的方法。随着信息技术的不断发展,如何实现大容量信息的存储和编码是当前光电子领域广泛关注的一个问题。Metasurface material is a new type of nanomaterial composed of arrays of subwavelength structures and capable of super-tuning light waves. Its appearance provides a new method for realizing the miniaturization, integration and high performance of optoelectronic devices. With the continuous development of information technology, how to realize the storage and encoding of large-capacity information is a problem that is widely concerned in the field of optoelectronics.

为了增加器件信息容量和提升器件功能性,许多基于超表面材料的多通道信息编码方法被相继提出,按照纳米结构的类型划分,大体上可以分为三类:1)基于变转角纳米结构的多通道信息编码方法;2)基于变大小纳米结构的多通道信息编码方法;3)基于变转角加变大小纳米结构的多通道信息编码方法。In order to increase the information capacity of the device and improve the functionality of the device, many multi-channel information encoding methods based on metasurface materials have been proposed one after another. According to the type of nanostructure, they can be roughly divided into three categories: 1) Multi-channel information encoding methods based on variable-angle nanostructures Channel information coding method; 2) Multi-channel information coding method based on variable size nanostructure; 3) Multi-channel information coding method based on variable rotation angle and variable size nanostructure.

目前基于变大小纳米结构或者变大小加转角纳米结构的编码方法都对加工要求比较高,而基于变转角纳米结构的编码方法多以牺牲图像的质量来换取编码的通道数,从本质上来说,信息容量并没有得到提升。本文基于变转角纳米结构,提出了一种三通道信息编码的方法。At present, the encoding methods based on variable-size nanostructures or variable-size-plus-angle nanostructures have relatively high processing requirements, while encoding methods based on variable-angle nanostructures often sacrifice image quality in exchange for the number of encoding channels. Essentially, Information capacity has not been improved. In this paper, a three-channel information encoding method is proposed based on variable-angle nanostructures.

发明内容Contents of the invention

鉴于现有技术存在的问题,本发明的目的在于提供一种利用新型光学薄膜实现多通道信息编码的方法,通过巧妙的设计新型光学薄膜中纳米结构的转向角,能够实现三通道信息之间的转换,在高端防伪、偏振显示、图像隐藏等领域具有很好的发展前景。In view of the problems existing in the prior art, the purpose of the present invention is to provide a method for realizing multi-channel information encoding by using a new type of optical film. By ingeniously designing the steering angle of the nanostructure in the new type of optical film, the information between the three channels can be realized. Conversion, has a good development prospect in the fields of high-end anti-counterfeiting, polarization display, image hiding and so on.

本发明提供了一种利用新型光学薄膜实现多通道信息编码的方法,包括如下步骤:The invention provides a method for realizing multi-channel information encoding by using a novel optical film, which includes the following steps:

1)构建纳米结构单元;所述纳米结构单元包括透明基底和沉淀在基底工作面上的纳米砖,以结构单元直角边为x轴和y轴建立xoy坐标系,所述纳米砖长边为长轴、短边为短轴,所述纳米砖的长轴与x轴夹角为纳米砖的转向角θ;1) Build a nanostructure unit; the nanostructure unit includes a transparent base and a nano-brick deposited on the base working surface, and the xoy coordinate system is established with the right-angled side of the structural unit as the x-axis and the y-axis, and the long side of the nano-brick is the length The axis and the short side are short axes, and the angle between the long axis of the nano-brick and the x-axis is the steering angle θ of the nano-brick;

2)根据入射光波长λ优化所述纳米结构单元的结构参数,所述结构参数包括:所述基底工作面的边长C以及所述纳米砖的长轴L、短轴W、高度H;2) optimize the structural parameters of the nanostructure unit according to the incident light wavelength λ, the structural parameters include: the side length C of the base working surface and the long axis L, short axis W, and height H of the nano bricks;

3)构建纳米结构阵列,所述纳米结构阵列包含多个纳米结构单元;设定以偏振方向α1=π/2的线偏振光入射至所述纳米结构阵列再经过以透光轴方向α2=0的检偏器,能够在纳米结构阵列编码第一幅图像;偏振方向保持不变的线偏振光入射至所述纳米结构阵列再经过以透光轴方向至α2=π/4的检偏器,能够在纳米结构阵列表面编码第二幅图像;偏正方向α1=-π/8的线偏振光入射至所述纳米结构阵列再经过以透光轴方向α2=π/8的检偏器,能够在纳米结构阵列表面编码第三幅图像,即在一个变转角纳米结构组成的阵列上,实现三幅图的同时编码。3) Construct a nanostructure array, the nanostructure array includes a plurality of nanostructure units; set the linearly polarized light with the polarization direction α 1 = π/2 to enter the nanostructure array and then pass through the light transmission axis direction α 2 = 0, the first image can be encoded in the nanostructure array; the linearly polarized light whose polarization direction remains unchanged enters the nanostructure array and then passes through the detector in the direction of the transmission axis to α 2 =π/4 A polarizer, capable of encoding the second image on the surface of the nanostructure array; the linearly polarized light in the polarization direction α 1 =-π/8 is incident on the nanostructure array and then passes through the light transmission axis direction α 2 =π/8 The analyzer can encode the third image on the surface of the nanostructure array, that is, on an array composed of nanostructures with variable rotation angles, the simultaneous encoding of three images can be realized.

进一步地,1)步骤中所述的透明基底为熔融石英玻璃材料,所述的纳米砖为金、银、铝或硅材料。Further, the transparent substrate in step 1) is fused silica glass material, and the nano bricks are gold, silver, aluminum or silicon material.

进一步地,2)步骤中纳米结构单元的结构参数是根据选定的所述入射光波长λ,通过电磁仿真优化得到。Further, the structural parameters of the nanostructure unit in the step 2) are obtained through electromagnetic simulation optimization according to the selected wavelength λ of the incident light.

进一步地,3)步骤中纳米结构阵列中每个纳米结构单元都等效为一个起偏器,当线偏光经过纳米砖起偏器,再经过检偏器后,出射光强可由表示为:Further, in step 3), each nanostructure unit in the nanostructure array is equivalent to a polarizer. When the linearly polarized light passes through the nanobrick polarizer and then the analyzer, the outgoing light intensity can be expressed as:

Figure BDA0003038359230000021
Figure BDA0003038359230000021

式中:I0为入射偏振光的强度,θ为纳米砖的转向角,α1为入射线偏振光的偏振方向,α2为检偏器的透光轴方向;In the formula: I 0 is the intensity of the incident polarized light, θ is the steering angle of the nano-brick, α 1 is the polarization direction of the incident ray polarized light, and α 2 is the transmission axis direction of the analyzer;

a、入射线偏光的偏振方向和检偏器的透光轴垂直(α2=α1+π/2),出射光强可以简化为:a. The polarization direction of the incident ray polarized light is perpendicular to the transmission axis of the analyzer (α 21 +π/2), and the output light intensity can be simplified as:

Figure BDA0003038359230000031
Figure BDA0003038359230000031

其中通过调节纳米砖的转向角θ,可以实现出射强度的连续调节;入射光偏振方向α1=π/2、α2=0时,出射光强为Among them, by adjusting the steering angle θ of the nano-bricks, the continuous adjustment of the outgoing intensity can be realized; when the polarization direction of the incident light is α1=π/2, α2=0, the outgoing light intensity is

Figure BDA0003038359230000032
Figure BDA0003038359230000032

b、入射线偏光的偏振方向α1=π/2,检偏器的透光轴方向α2=π/4时,出射光强可以简化为b. When the polarization direction of the incident ray polarization is α 1 = π/2, and the direction of the transmission axis of the analyzer is α 2 = π/4, the outgoing light intensity can be simplified as

Figure BDA0003038359230000033
Figure BDA0003038359230000033

c、入射线偏光的偏振方向α1=-π/8,检偏器的透光轴方向α2=π/8时,出射光强可以简化为c. When the polarization direction of the incident ray polarization is α 1 =-π/8, and the direction of the transmission axis of the analyzer is α 2 =π/8, the outgoing light intensity can be simplified as

Figure BDA0003038359230000034
Figure BDA0003038359230000034

进一步地,三种出射光强度调制函数在纳米砖的转向角θ取值范围[0,π]的强度变化关系为:Further, the intensity variation relationship of the three kinds of outgoing light intensity modulation functions in the value range [0, π] of the steering angle θ of the nano-bricks is:

a.纳米砖的转向角θ在[0,π/8]范围内变动时,其对应的强度I1能够实现0-0.5的连续调制,I2的强度小于0.5,I3的强度大于0.5;a. When the steering angle θ of the nano-brick changes in the range of [0, π/8], its corresponding intensity I 1 can realize continuous modulation of 0-0.5, the intensity of I 2 is less than 0.5, and the intensity of I 3 is greater than 0.5;

b.纳米砖的转向角θ在[3π/8,π/2]范围内变动时,其对应的强度I1也能够实现0-0.5的连续调制,I2的强度大于0.5,I3的强度小于0.5;b. When the steering angle θ of nanobricks changes within the range of [3π/8,π/2], the corresponding intensity I 1 can also achieve continuous modulation from 0-0.5, the intensity of I 2 is greater than 0.5, and the intensity of I 3 less than 0.5;

c.纳米砖的转向角θ在[π/2,5π/8]范围内变动时,其对应的强度仍然能够实现0-0.5的连续调制,I2的强度大于0.5,I3的强度大于0.5;c. When the steering angle θ of nanobricks changes in the range of [π/2,5π/8], its corresponding intensity can still achieve continuous modulation of 0-0.5, the intensity of I 2 is greater than 0.5, and the intensity of I 3 is greater than 0.5 ;

d.纳米砖的转向角θ在[7π/8,π]范围内变动时,其对应的强度仍然能够实现0-0.5的连续调制,I2的强度小于0.5,I3的强度小于0.5;d. When the steering angle θ of the nano-brick changes in the range of [7π/8,π], its corresponding intensity can still achieve continuous modulation of 0-0.5, the intensity of I 2 is less than 0.5, and the intensity of I 3 is less than 0.5;

通过合理的排布纳米砖的转向角,能够在一片超表面上同时实现对三幅图像的编码。By rationally arranging the steering angles of nanobricks, three images can be encoded simultaneously on one metasurface.

进一步地,新型薄膜为不同转角、相同尺寸的纳米砖,其中纳米砖为微纳起偏器,能够反射或者透射沿着纳米砖长轴入射的线偏光,同时透射或者反射沿着纳米砖短轴入射的线偏振光。Furthermore, the new film is nano-bricks with different corners and the same size, in which the nano-bricks are micro-nano polarizers, which can reflect or transmit linearly polarized light incident along the long axis of the nano-bricks, and at the same time transmit or reflect light along the short axis of the nano-bricks. Incident linearly polarized light.

进一步地,第一幅图像为连续灰度图像,第二幅图像和第三幅图像均为二值图像。Further, the first image is a continuous grayscale image, and both the second image and the third image are binary images.

与现有技术相比较,本发明的有益效果:Compared with prior art, the beneficial effect of the present invention:

1)采用本发明的技术方案,变转角纳米结构阵列在不同偏振状态下形成的三幅图像可分别设计,其中通道1和通道2的图像没有任何相关性,无法相互推断,可以任意设计,通道3的图像与通道1的图像没有关联,与通道2图像有关联,但三个通道之间可以通过转动起偏器和检偏器实现转换,因此可以应用于偏振显示、加密、高端防伪等领域,为未来的安全技术提供一种新的方法和途径;1) By adopting the technical solution of the present invention, the three images formed by the variable-angle nanostructure array under different polarization states can be designed separately, wherein the images of channel 1 and channel 2 have no correlation and cannot be inferred from each other, and can be designed arbitrarily. The image of 3 is not related to the image of channel 1, but is related to the image of channel 2, but the conversion between the three channels can be realized by rotating the polarizer and analyzer, so it can be used in polarization display, encryption, high-end anti-counterfeiting and other fields , to provide a new method and approach for future security technology;

2)本发明的设计方法提出了一个新的光波操控的自由度,设计方法巧妙,加工难度低,所用结构简单,仅仅需要一种纳米砖结构单元便实现了三种纳米印刷图像的编码,因此本发明所设计的超表面体积小、重量轻、可高度集成,适应于未来小型化、微型化的发展;2) The design method of the present invention proposes a new degree of freedom of light wave manipulation, the design method is ingenious, the processing difficulty is low, the structure used is simple, and only one nano-brick structural unit is needed to realize the encoding of three nano-printed images, so The metasurface designed by the present invention is small in size, light in weight, highly integrated, and suitable for the development of miniaturization and miniaturization in the future;

3)本发明所生产的第一通道图像为连续灰度图像,第二通道和第三通道为二值图像,图案可以任意生成,解码条件不一样,不易于被模仿和伪造,因此用户可以应用于高端手表,奢侈品、芯片等需要防伪的器件;3) The first channel image produced by the present invention is a continuous grayscale image, the second channel and the third channel are binary images, the pattern can be generated arbitrarily, the decoding conditions are different, and it is not easy to be imitated and forged, so users can apply For high-end watches, luxury goods, chips and other devices that require anti-counterfeiting;

4)本发明的新型光学薄膜既可以在透射模式下工作,也可以在反射模式下工作。4) The novel optical film of the present invention can work both in the transmission mode and in the reflection mode.

附图说明Description of drawings

图1是本实施例中纳米砖结构单元示意图;Fig. 1 is the schematic diagram of nano-brick structural unit in the present embodiment;

图2是本实施例中纳米结构单元透反射率扫描图;Fig. 2 is the scanning diagram of the transmittance and reflectance of the nanostructure unit in the present embodiment;

图3是本实施例中强度调制函数与纳米砖转向角关系的示意图;Fig. 3 is a schematic diagram of the relationship between the intensity modulation function and the steering angle of nano bricks in the present embodiment;

图4是本实施例中设计的第一通道的连续灰度纳米印刷图像;Fig. 4 is the continuous grayscale nanoprinting image of the first channel designed in the present embodiment;

图5是本实施例中设计的第二通道的二值图像;Fig. 5 is the binary image of the second channel designed in the present embodiment;

图6是本实施例中设计的第三通道的二值图像。Fig. 6 is a binary image of the third channel designed in this embodiment.

具体实施方式Detailed ways

下面结合实施例对本发明作进一步的说明,但本发明所保护的范围不限于所述范围。The present invention will be further described below in conjunction with the examples, but the protection scope of the present invention is not limited to the said scope.

实施例1Example 1

一种利用新型光学薄膜实现多通道信息编码的方法,具体步骤如下:A method for realizing multi-channel information encoding by using a novel optical film, the specific steps are as follows:

首先,构建纳米结构单元,如图1所示,纳米单元结构由银纳米砖,硅基底层构成,其次,选取设计波长为λ=633nm,针对该波长,通过电磁仿真软件CST对纳米转结构单元进行优化仿真,得到优化后的硅纳米砖的尺寸参数为:长为L=130nm,宽为W=85nm,高为H=70nm,单元结构基底边长为C=400nm。First, construct the nano-structure unit, as shown in Figure 1, the nano-unit structure is composed of silver nano-bricks and a silicon base layer, and secondly, select the design wavelength as λ=633nm, for this wavelength, use the electromagnetic simulation software CST to convert the nano-structure unit The optimization simulation is carried out, and the size parameters of the optimized silicon nano-bricks are: the length is L=130nm, the width is W=85nm, the height is H=70nm, and the side length of the unit structure base is C=400nm.

该结构参数下纳米砖对沿着纳米砖长轴和短轴入射的线偏振光的透反射效率如图2所示,其中Rl、Rs分别代表沿纳米砖长轴和短轴反射的反射光效率,其中Tl、Ts分别代表沿纳米砖长轴和短轴透射的透射光效率。 The transmission and reflection efficiency of nanobricks for linearly polarized light incident along the long and short axes of nanobricks under this structural parameter is shown in Fig . Light efficiency, where T l and T s represent the transmitted light efficiency along the long axis and short axis of the nanobrick, respectively.

由图2可知,在工作波长633nm下,Rl高达80%,Rs被抑制到1%以下,Ts在90%以上,Tl被抑制到1%以下,表明沿着纳米砖长轴入射的光基于全部被反射,沿着纳米砖短轴入射的光几乎全部被透射,因此该优化后纳米砖单元结构可以实现偏振分光的功能,也即是透射式起偏器和反射式起偏器。It can be seen from Figure 2 that at the working wavelength of 633nm, R l is as high as 80%, R s is suppressed below 1%, T s is above 90%, and T l is suppressed below 1%, indicating that the incident along the long axis of the nanobrick The light is completely reflected, and the light incident along the short axis of the nano-brick is almost completely transmitted. Therefore, the optimized nano-brick unit structure can realize the function of polarization splitting, that is, a transmissive polarizer and a reflective polarizer. .

最后构建纳米结构阵列,所述纳米结构阵列包含多个纳米结构单元,当线偏振光入射光经过纳米结构阵列,再经过检偏器后,通过改变其起偏器和检偏器的透光轴方向,可以得到不同的光强调制函数,其与纳米砖方位角的变换关系图如图3所示,当纳米砖的方位角在[0,π/8]范围内变动(区域#1)时,其对应的强度I1能够实现0-0.5的连续调制、I2的强度小于0.5、I3的强度大于0.5;当纳米砖的方位角在[3π/8,π/2]范围内变动(区域#2)时,其对应的强度I1也能够实现0-0.5的连续调制、I2大于0.5,I3的强度小于0.5。当纳米砖的方位角在[π/2,5π/8]范围内变动(区域#3)时,其对应的强度仍然能够实现0-0.5的连续调制,I2大于0.5,I3的强度大于0.5。纳米砖的方位角在[7π/8,π]范围内变动(区域#4)时,其对应的强度仍然能够实现0-0.5的连续调制,I2小于0.5,I3的强度小于0.5。因此基于这个原理,可以在一个结构表面同时设计生成三幅图像,如图4所示的一幅连续灰度图像,如图5和图6所示的两幅二值图像。Finally, a nanostructure array is constructed. The nanostructure array contains a plurality of nanostructure units. When the linearly polarized incident light passes through the nanostructure array and then the analyzer, the light transmission axis of the polarizer and the analyzer is changed. direction, different light intensity modulation functions can be obtained, and the transformation relationship between it and the azimuth angle of the nano-brick is shown in Figure 3. When the azimuth angle of the nano-brick changes in the range of [0, π/8] (area #1) , the corresponding intensity I 1 can realize the continuous modulation of 0-0.5, the intensity of I 2 is less than 0.5, and the intensity of I 3 is greater than 0.5; when the azimuth angle of the nano brick changes in the range of [3π/8, π/2] ( In region #2), its corresponding intensity I 1 can also achieve continuous modulation of 0-0.5, I 2 is greater than 0.5, and the intensity of I 3 is less than 0.5. When the azimuth angle of the nanobrick varies in the range of [π/2,5π/8] (region #3), its corresponding intensity can still achieve continuous modulation from 0 to 0.5, I 2 is greater than 0.5, and the intensity of I 3 is greater than 0.5. When the azimuth angle of nanobricks varies in the range of [7π/8, π] (region #4), its corresponding intensity can still achieve continuous modulation from 0-0.5, and the intensity of I 2 is less than 0.5, and the intensity of I 3 is less than 0.5. Therefore, based on this principle, three images can be designed and generated on a structured surface at the same time, a continuous grayscale image as shown in Figure 4, and two binary images as shown in Figures 5 and 6.

Claims (3)

1.一种利用新型光学薄膜实现多通道信息编码的方法,其特征在于包括如下步骤:1. A method utilizing novel optical film to realize multi-channel information encoding, characterized in that it comprises the steps: 1)构建纳米结构单元;所述纳米结构单元包括透明基底和沉淀在基底工作面上的纳米砖,以结构单元直角边为x轴和y轴建立xoy坐标系,所述纳米砖长边为长轴、短边为短轴,所述纳米砖的长轴与x轴夹角为纳米砖的转向角θ;1)步骤中所述的透明基底为熔融石英玻璃材料,所述的纳米砖为金、银、铝或硅材料;1) Build a nano-structure unit; the nano-structure unit includes a transparent substrate and a nano-brick deposited on the base working surface, and the x-axis and the y-axis set up a xoy coordinate system with the right-angled side of the structural unit, and the long side of the nano-brick is long Axes and short sides are short axes, and the angle between the long axis and the x-axis of the nano-bricks is the steering angle θ of the nano-bricks; 1) the transparent substrate described in the step is a fused silica glass material, and the nano-bricks are gold , silver, aluminum or silicon materials; 2)根据入射光波长λ优化所述纳米结构单元的结构参数,所述结构参数包括:所述基底工作面的边长C以及所述纳米砖的长轴L、短轴W、高度H;2) Optimizing the structural parameters of the nanostructure unit according to the incident light wavelength λ, the structural parameters include: the side length C of the base working surface and the long axis L, short axis W, and height H of the nano bricks; 3)构建纳米结构阵列,所述纳米结构阵列包含多个纳米结构单元;设定以偏振方向α1=π/2的线偏振光入射至所述纳米结构阵列再经过以透光轴方向α2=0的检偏器,能够在纳米结构阵列编码第一幅图像;偏振方向保持不变的线偏振光入射至所述纳米结构阵列再经过以透光轴方向至α2=π/4的检偏器,能够在纳米结构阵列表面编码第二幅图像;偏振方向α1=-π/8的线偏振光入射至所述纳米结构阵列再经过以透光轴方向α2=π/8的检偏器,能够在纳米结构阵列表面编码第三幅图像,即在一个变转角纳米结构组成的阵列上,实现三幅图的同时编码;3) Construct a nanostructure array, the nanostructure array includes a plurality of nanostructure units; set the linearly polarized light with the polarization direction α 1 = π/2 to enter the nanostructure array and then pass through the light transmission axis direction α 2 = 0, the first image can be encoded in the nanostructure array; the linearly polarized light whose polarization direction remains unchanged enters the nanostructure array and then passes through the detector in the direction of the transmission axis to α 2 =π/4 The polarizer can encode the second image on the surface of the nanostructure array; the linearly polarized light with the polarization direction α 1 =-π/8 is incident on the nanostructure array and passes through the detector with the transmission axis direction α 2 =π/8 The polarizer can encode the third image on the surface of the nanostructure array, that is, on an array composed of nanostructures with variable rotation angles, the simultaneous encoding of three images can be realized; 3)步骤中纳米结构阵列中每个纳米结构单元都等效为一个起偏器,当线偏振光经过纳米砖起偏器,再经过检偏器后,出射光强可表示为:3) In the step, each nanostructure unit in the nanostructure array is equivalent to a polarizer. When the linearly polarized light passes through the nanobrick polarizer and then the analyzer, the emitted light intensity can be expressed as:
Figure FDA0003926535150000021
Figure FDA0003926535150000021
式中:I0为入射偏振光的强度,θ为纳米砖转向角,α1为入射线偏振光的偏振方向,α2为检偏器的透光轴方向;In the formula: I 0 is the intensity of the incident polarized light, θ is the nanobrick steering angle, α 1 is the polarization direction of the incident ray polarized light, and α 2 is the transmission axis direction of the analyzer; a、入射线偏振光的偏振方向和检偏器的透光轴垂直α2=α1+π/2,出射光强可以简化为:a. The polarization direction of the incident linearly polarized light is perpendicular to the transmission axis of the analyzer α 21 +π/2, and the output light intensity can be simplified as:
Figure FDA0003926535150000022
Figure FDA0003926535150000022
其中通过调节纳米砖的转向角θ,可以实现出射强度的连续调节;入射光偏振方向α1=π/2、α2=0时,出射光强为The output intensity can be continuously adjusted by adjusting the steering angle θ of the nano-bricks; when the incident light polarization direction α 1 =π/2, α 2 =0, the output light intensity is
Figure FDA0003926535150000023
Figure FDA0003926535150000023
b、入射线偏振光的偏振方向α1=π/2,检偏器的透光轴方向α2=π/4时,出射光强可以简化为b. When the polarization direction of the incident ray polarized light is α 1 = π/2, and the direction of the transmission axis of the analyzer is α 2 = π/4, the outgoing light intensity can be simplified as
Figure FDA0003926535150000024
Figure FDA0003926535150000024
c、入射线偏振光的偏振方向α1=-π/8,检偏器的透光轴方向α2=π/8时,出射光强可以简化为c. When the polarization direction of the incident ray polarized light is α 1 =-π/8, and the transmission axis direction of the analyzer is α 2 =π/8, the exit light intensity can be simplified as
Figure FDA0003926535150000025
Figure FDA0003926535150000025
三种出射光强度调制函数在纳米砖的转向角θ取值范围[0,π]的强度变化关系为:The intensity variation relationship of the three outgoing light intensity modulation functions in the range [0, π] of the steering angle θ of the nano-bricks is: a.纳米砖的转向角θ在[0,π/8]范围内变动时,其对应的强度I1能够实现0-0.5的连续调制,I2的强度小于0.5,I3的强度大于0.5;a. When the steering angle θ of the nano-brick changes in the range of [0, π/8], its corresponding intensity I 1 can realize continuous modulation of 0-0.5, the intensity of I 2 is less than 0.5, and the intensity of I 3 is greater than 0.5; b.纳米砖的转向角θ在[3π/8,π/2]范围内变动时,其对应的强度I1也能够实现0-0.5的连续调制,I2的强度大于0.5,I3的强度小于0.5;b. When the steering angle θ of nanobricks changes within the range of [3π/8,π/2], the corresponding intensity I 1 can also achieve continuous modulation from 0-0.5, the intensity of I 2 is greater than 0.5, and the intensity of I 3 less than 0.5; c.纳米砖的转向角θ在[π/2,5π/8]范围内变动时,其对应的强度I1仍然能够实现0-0.5的连续调制,I2的强度大于0.5,I3的强度大于0.5;c. When the steering angle θ of the nano brick changes in the range of [π/2,5π/8], its corresponding intensity I 1 can still achieve continuous modulation of 0-0.5, the intensity of I 2 is greater than 0.5, and the intensity of I 3 Greater than 0.5; d.纳米砖的转向角θ在[7π/8,π]范围内变动时,其对应的强度I1仍然能够实现0-0.5的连续调制,I2的强度小于0.5,I3的强度小于0.5;d. When the steering angle θ of nanobricks changes within the range of [7π/8,π], the corresponding intensity I 1 can still achieve continuous modulation from 0-0.5, the intensity of I 2 is less than 0.5, and the intensity of I 3 is less than 0.5 ; 通过合理的排布纳米砖的转向角,能够在一片超表面上同时实现对三幅图像的编码;By rationally arranging the steering angle of nano-bricks, three images can be encoded simultaneously on one metasurface; 新型光学薄膜为不同转角、相同尺寸的纳米砖,其中纳米砖为微纳起偏器,能够反射或者透射沿着纳米砖长轴入射的线偏振光,同时透射或者反射沿着纳米砖短轴入射的线偏振光。The new optical film is nano-bricks with different rotation angles and the same size. The nano-bricks are micro-nano polarizers, which can reflect or transmit linearly polarized light incident along the long axis of the nano-brick, and at the same time transmit or reflect the incident light along the short axis of the nano-brick. of linearly polarized light.
2.根据权利要求1所述的一种利用新型光学薄膜实现多通道信息编码的方法,其特征在于2)步骤中纳米结构单元的结构参数是根据选定的所述入射光波长λ,通过电磁仿真优化得到。2. A method for utilizing novel optical thin films to realize multi-channel information encoding according to claim 1, characterized in that 2) the structural parameters of the nanostructure unit in the step are based on the selected incident light wavelength λ, by electromagnetic The simulation optimization is obtained. 3.根据权利要求1所述的一种利用新型光学薄膜实现多通道信息编码的方法,其特征在于第一幅图像为连续灰度图像,第二幅图像和第三幅图像均为二值图像。3. A method of utilizing novel optical films to realize multi-channel information encoding according to claim 1, characterized in that the first image is a continuous grayscale image, and the second image and the third image are binary images .
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Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109814195A (en) * 2019-03-29 2019-05-28 武汉邮电科学研究院有限公司 Multi-functional super surface texture, super surface element and encryption method based on polarization
CN110335533A (en) * 2019-06-19 2019-10-15 武汉大学 An Optical Information Hiding Method Based on Metasurface Array Structure
CN111399088A (en) * 2020-03-25 2020-07-10 武汉大学 Three-channel image display method based on micro-nano polarizer array super-surface

Family Cites Families (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10310287B2 (en) * 2013-10-28 2019-06-04 Ramot At Tel-Aviv University Ltd. System and method for controlling light by an array of optical resonators
KR102049749B1 (en) * 2018-03-22 2020-01-08 포항공과대학교 산학협력단 Dielectric based metasurface hologram device and manufacturing method thereof and display device having the same
US11333798B2 (en) * 2018-07-06 2022-05-17 The Regents Of The University Of Michigan Compound metaoptics for amplitude and phase control of wavefronts
CN110568557B (en) * 2019-08-13 2020-09-22 武汉大学 Information multiplexing method based on polarization control
CN111127289B (en) * 2019-12-18 2022-02-01 武汉大学 Design method of high-low frequency multiplexing super-surface anti-counterfeiting image with watermark
CN111008948B (en) * 2019-12-18 2022-10-11 武汉大学 Method for combining random pattern with space-frequency multiplexing super-surface image
CN111007583B (en) * 2019-12-23 2020-11-17 武汉大学 Design method of three-channel anti-counterfeiting metasurface
CN111145071B (en) * 2019-12-23 2021-10-22 武汉大学 A three-channel metasurface multiplexing method for superimposing watermarks in continuous grayscale images
CN111292226B (en) * 2020-01-15 2021-11-16 武汉大学 Design method for realizing multiplexing of structural color image and continuous gray level image based on super surface
CN111210713B (en) * 2020-01-21 2021-09-03 武汉大学 Anti-counterfeiting shading and image multiplexing-based anti-counterfeiting super surface design method

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109814195A (en) * 2019-03-29 2019-05-28 武汉邮电科学研究院有限公司 Multi-functional super surface texture, super surface element and encryption method based on polarization
CN110335533A (en) * 2019-06-19 2019-10-15 武汉大学 An Optical Information Hiding Method Based on Metasurface Array Structure
CN111399088A (en) * 2020-03-25 2020-07-10 武汉大学 Three-channel image display method based on micro-nano polarizer array super-surface

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